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Neutrino Oscillations 4 March 08 Introduction: Neutrinos • A neutrino (ν) is an elementary particle, one of the fundamental constituents of matter. It has almost no mass,…
Neutrino Oscillations Suggested reading: C. Giunti and C.W. Kim, Fundamentals of Neutrino Physics and Astrophysics, Oxford University Press (2007; 728 pages) Elisa Bernardini…
Cellular kinetics and associated reactor design: Modelling Cell Growth CP504 – Lecture 8 Approaches to modelling cell growth Unstructured segregated models Substrate inhibited…
New Ideas in Long Range Reactor Monitoring with Neutrinos John G. Learned and Stephen T. Dye Dept. of Physics and Astronomy University of Hawaii Introduction Previously we…
Modelling Cell Growth Cellular kinetics and associated reactor design:CP504 – Lecture 8 Cellular kinetics and associated reactor design: Modelling Cell Growth Approaches…
Slide 1 μ Reactor Synthesis of Nano-Particles Interest in Nano-Particles μReactor versus Batch Reactor Eric Hostetler, Joe Ferron, Mohammad Al Falasi Project Advisor: Dr.…
Sensitivity and Uncertainty Analysis of Coupled Reactor Physics Problems Method Development for Multi-Physics in Reactors Zoltán Perkó Sensitivity and U ncertainty A nalysis…
1. Neutrino Oscillation 1. Neutrino Oscillation 1 2 3 θ13 θ12 θ23 θ12 θ13 θ23 Gaol of RENO experiment = θ13 1. Neutrino Oscillation νe νe νe νe νe Distance Probability…
Microsoft PowerPoint - Kearns-NUSS2007-Neutrino-Detectors-I-print.pptNeutrino Detectors I Inverse Beta Decay Tracking Detectors Two ν Experiment NuTeV, MINOS,
Motivation ν masses from ν oscillation are a clear signature of physics beyond SM access to very high new physics scale (M NP ) Oscillation parametrized with neutrino
Long-range programme in neutrino physics: superbeam, β beam, neutrino factory Complementary programme in μ physics: rare μ decays, μ properties, μ colliders? Next-generation…
Determination of Planck’s constant using photo-cell Theory: From Einstein’s photoelectric equation, we know hυ = hυ 0 + 1 2 mv 2 = hυ 0 +eV s =¢ + eV s Where, υ=…
Rutherford - atoms have nuclei Stern - μp = (1+κp)(e/2M) Hofstadter - nuclei are not point-like, rather high density core and sparse surrounding Mott - light point-like
structureDr Michael Thrippleton •through space •1D NOE •2D NOESY Relaxation is the process by which magnetisation returns to equilibrium • longitudinal
15th August 2019 →Υ(4S)→BS)→BB Produce only BB pair in quantum- entangled state – CESR/CLEO 1979-2001 – PEP-II/BaBar 1999-2008 –
Microsoft PowerPoint - zuber.pptKai Zuber, University of Sussex Workshop Astroteilchenphysik, DESY Zeuthen 4.-.5.10.2005 How to explain all other double beta proposals in
Experimental facility HiPER 4a operation in bunch mode for scientific viability 3 Neutron Flux γ-rays Dose Thermal annealing Silica Final Lenses under HIPER Laser Fusion…
High precision measurement of θ13 : Progress of Daya Bay reactor antineutrino experiment Zhimin Wang IHEP China On behalf of Daya Bay collaboration NuFact’11 1st~6th Aug…
reconstructed vT candidate event Caren Hagner, Universität Hamburg DESY Seminar, 12.10.2010 VARIABLE Value kink (mrad) 41 ± 2 decay length (mm) 1335 ± 35 P (daughter)…
NP08 Future beam options for ν experiments Yves Déclais 1 Future beam options for long baseline neutrino experiments Yves Déclais Université Lyon1 CNRSIN2P3IPNL NP08…